Dielectric constants of yttrium and rare-earth garnets, the polarizability of gallium oxide, and the oxide additivity rule
Abstract
The dielectric constants (kappa[script ']) and dielectric loss values of 10 rare-earth gallium garnets and 1 rare-earth aluminum garnet were measured at 1 MHz using a two-terminal method with empirically determined edge corrections. The results are: kappa[script '](Dy3Al5O12)=11.07±0.05; kappa[script '](Ho3Ga5O12) =12.38±0.05; kappa[script '](Dy3Ga5O12)=12.36±0.06; kappa[script '](Tb3Ga5O12) =12.40 ±0.03; kappa[script '](Gd3Ga5O12) =12.18±0.10; kappa[script '](Eu3Ga5O12) =12.46±0.05; kappa[script '](Sm3Ga5O12) =12.55±0.03; kappa[script '](Nd3Ga5O12) =12.59±0.12; kappa[script '](Y3Sc2Ga3O12) =12.94±0.03; kappa[script '](Sm3Sc2Ga3O12) =13.67±0.04; and kappa[script '](La2.66Lu2.66Ga2.66O12) =14.40±0.03. The dielectric polarizability of Ga2O3 derived from the dielectric constants of these and other Ga compounds is 8.80±0.14 Å3. The agreement between measured dielectric polarizabilities as determined from the Clausius–Mosotti equation and those calculated from the sum of oxide polarizabilities according to alphaD(mineral) =SigmaalphaD (oxides) for six aluminum garnets and twelve gallium garnets is ~1%.
Additional Information
Copyright © 1990 American Institute of Physics (Received 13 November 1989; accepted 9 January 1990) We thank D. Appleman of the Smithsonian Institution for the crystals of Eu3Ga5O12 (USNM 53), Tb3Ga5O12 (USNM 87), and Nd3Ga5O12 (USNM 92), R.W. Shiffer for sample preparation and R.A. Oswald for making capacitance measurements, and A. BRown (Studvik Energiteknik AB, Nykoping, Sweden) and C. Fortis for obtaining cell dimensions of Ho3Al5O12, Y1.5Er1.5Al5O12 and Gd3Sc2Al3O12. This work was supported in part by National Science Foundation Grant No. EAR 86-18200.Files
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- CaltechAUTHORS:SHAjap90
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2006-12-12Created from EPrint's datestamp field
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2021-11-08Created from EPrint's last_modified field
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